Let $ \mathbb{R} $ denote the set of all real numbers. Define the function $ f: \mathbb{R} \to \mathbb{R} $ by $$ f(x) = \begin{cases} 2 - 2x^2 - x^2 \sin\left(\frac{1}{x}\right), & \text{if } x \ne 0, \\ 2, & \text{if } x = 0. \end{cases} $$ Then which one of the following statements is TRUE?
\( x = 0 \) is a point of local minima of \( f \)
Step 1: Analyze continuity at \( x = 0 \) \[ \lim_{x \to 0} f(x) = \lim_{x \to 0} \left[2 - 2x^2 - x^2 \sin\left(\frac{1}{x}\right)\right] \] Since \( -1 \le \sin\left(\frac{1}{x}\right) \le 1 \), \[ - x^2 \le x^2 \sin\left(\frac{1}{x}\right) \le x^2 \Rightarrow -x^2 \le -x^2 \sin\left(\frac{1}{x}\right) \le x^2 \] \[ -2x^2 - x^2 \le f(x) - 2 \le -2x^2 + x^2 \Rightarrow -3x^2 \le f(x) - 2 \le -x^2 \Rightarrow \lim_{x \to 0} f(x) = 2 \] So, \( f \) is continuous at \( x = 0 \).
Step 2: Check differentiability at \( x = 0 \) Let’s analyze: \[ f(x) = 2 - 2x^2 - x^2 \sin\left(\frac{1}{x}\right) \Rightarrow f'(x) = -4x - 2x \sin\left(\frac{1}{x}\right) + \cos\left(\frac{1}{x}\right) \] Here, \( \cos\left(\frac{1}{x}\right) \) oscillates as \( x \to 0 \) and does not converge. Hence, \( f \) is not differentiable at \( x = 0 \).
Step 3: Examine local extrema We check the behavior of \( f(x) \) around 0: \[ f(x) = 2 - 2x^2 - x^2 \sin\left(\frac{1}{x}\right) \le 2 - x^2<2 = f(0) \Rightarrow f(x)<f(0) \text{ near } x = 0 \] So, \( x = 0 \) is actually a local maximum, not a local minimum.
Step 4: Monotonicity Due to the oscillatory term \( \sin\left(\frac{1}{x}\right) \), the function is not monotonic in any neighborhood around 0. This rules out both strict increasing and decreasing nature in any interval \( (-\delta, 0) \) or \( (0, \delta) \).
Thus, the true statement is:
(C) For any positive real number \( \delta \), the function \( f \) is NOT an increasing function on the interval \( (-\delta, 0) \)
A solid glass sphere of refractive index $ n = \sqrt{3} $ and radius $ R $ contains a spherical air cavity of radius $ \dfrac{R}{2} $, as shown in the figure. A very thin glass layer is present at the point $ O $ so that the air cavity (refractive index $ n = 1 $) remains inside the glass sphere. An unpolarized, unidirectional and monochromatic light source $ S $ emits a light ray from a point inside the glass sphere towards the periphery of the glass sphere. If the light is reflected from the point $ O $ and is fully polarized, then the angle of incidence at the inner surface of the glass sphere is $ \theta $. The value of $ \sin \theta $ is ____
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity):
In a scattering experiment, a particle of mass $ 2m $ collides with another particle of mass $ m $, which is initially at rest. Assuming the collision to be perfectly elastic, the maximum angular deviation $ \theta $ of the heavier particle, as shown in the figure, in radians is:
A conducting square loop initially lies in the $ XZ $ plane with its lower edge hinged along the $ X $-axis. Only in the region $ y \geq 0 $, there is a time dependent magnetic field pointing along the $ Z $-direction, $ \vec{B}(t) = B_0 (\cos \omega t) \hat{k} $, where $ B_0 $ is a constant. The magnetic field is zero everywhere else. At time $ t = 0 $, the loop starts rotating with constant angular speed $ \omega $ about the $ X $ axis in the clockwise direction as viewed from the $ +X $ axis (as shown in the figure). Ignoring self-inductance of the loop and gravity, which of the following plots correctly represents the induced e.m.f. ($ V $) in the loop as a function of time: